Abstract:S I1 Einstein A-coefficientsEinstein A-coefficients for transitions among the 3s23p3 states of SII, calculated with the CIV3 code, are found to be up to -25% different from those of Mendoza and Zeippen. These new results are used to derive the theoretical emission line ratio R = 1(3s23p3 4S;iz-3s23p3 2D:/2)/ I(3s23p3 4S;/2-3s23p3 2D;/z) = I(6717 A)/1(6730A), which is a very useful electron density diagnostic for gaseous nebulae. The present diagnostin are up to 10% larger than those deduced using the A-values … Show more
“…Using the double-beam spectrograph mounted on the ANU 2.3 m telescope, Kingsburgh & English (1992) ple of Galactic PNe and found that electron densities derived from the two ratios were in excellent agreement. On the other hand, a very different result was obtained by Meatheringham & Dopita (1991) Aller et al 1996;Feibelman et al 1994Feibelman et al , 1996Hyung 1994;Hyung & Aller 1995a,b, 1996, 1997a,b, 1998Hyung et al 1993Hyung et al , 1994aHyung et al ,b,c, 1995Hyung et al , 1997Hyung et al , 1999aHyung et al ,b, 2000Hyung et al , 2001Keyes et al 1990;Keenan et al 1993Keenan et al , 1996Keenan et al , 1997 they determined simultaneously electron densities and temperatures using a number of plasma diagnostic lines in the optical and ultraviolet and found that overall the data yielded compatible and consistent results. More recently, Copetti & Writzl (2002), using data published in the literature, compared the observed line ratios for a number of density-diagnostics, instead of densities deduced from them, thus avoiding discarding measurements that yield ratios close to or beyond the the low-or high-N e limits.…”
Abstract. We present a comparison of electron densities derived from optical forbidden line diagnostic ratios for a sample of over a hundred nebulae. We consider four density indicators, theand [Ar ] λ4711/λ4740 doublet ratios. Except for a few H regions for which data from the literature were used, diagnostic line ratios were derived from our own high quality spectra. For the [O ] λ3729/λ3726 doublet ratio, we find that our default atomic data set, consisting of transition probabilities from Zeippen (1982)
“…Using the double-beam spectrograph mounted on the ANU 2.3 m telescope, Kingsburgh & English (1992) ple of Galactic PNe and found that electron densities derived from the two ratios were in excellent agreement. On the other hand, a very different result was obtained by Meatheringham & Dopita (1991) Aller et al 1996;Feibelman et al 1994Feibelman et al , 1996Hyung 1994;Hyung & Aller 1995a,b, 1996, 1997a,b, 1998Hyung et al 1993Hyung et al , 1994aHyung et al ,b,c, 1995Hyung et al , 1997Hyung et al , 1999aHyung et al ,b, 2000Hyung et al , 2001Keyes et al 1990;Keenan et al 1993Keenan et al , 1996Keenan et al , 1997 they determined simultaneously electron densities and temperatures using a number of plasma diagnostic lines in the optical and ultraviolet and found that overall the data yielded compatible and consistent results. More recently, Copetti & Writzl (2002), using data published in the literature, compared the observed line ratios for a number of density-diagnostics, instead of densities deduced from them, thus avoiding discarding measurements that yield ratios close to or beyond the the low-or high-N e limits.…”
Abstract. We present a comparison of electron densities derived from optical forbidden line diagnostic ratios for a sample of over a hundred nebulae. We consider four density indicators, theand [Ar ] λ4711/λ4740 doublet ratios. Except for a few H regions for which data from the literature were used, diagnostic line ratios were derived from our own high quality spectra. For the [O ] λ3729/λ3726 doublet ratio, we find that our default atomic data set, consisting of transition probabilities from Zeippen (1982)
“…Hibbert and co-workers have shown that two-electron promotions are important to include to get accurate energies, f -values and Einstein coefficients [63,64] 2 of the residual sulfur singly ionized ion were included in the close-coupling expansion. PI cross section calculations with this 512-level model were performed in the Dirac Coulomb approximation using the recently developed parallel version of the DARC codes [57,58].…”
Photoionization of the3s 2 3p 4 3 P and the 3s 2 3p 4 1 DPhotoionization of neutral atomic sulfur in the ground and metastable states was studied experimentally at a photon energy resolution of 44 meV FWHM. Relative cross section measurements were recorded by using tunable vacuum ultraviolet (VUV) radiation in the energy range 9 -30 eV obtained from a laser-produced plasma and the atomic species were generated by photolysis of molecular precursors. Photoionization of this atom is characterized by multiple Rydberg series of autoionizing resonances superimposed on a direct photoionization continuum. A wealth of resonance features observed in the experimental spectra are spectroscopically assigned and their energies and quantum defects tabulated. The cross-section measurements are compared with state-of-the-art theoretical cross-section calculations obtained from the Dirac Coulomb R-matrix method. Resonances series in the spectra are identified and compared indicating similar features in both the theoretical and experimental spectra.
“…Hibbert and co-workers have shown that two-electron promotions are important to include to get accurate energies, f -values and Einstein coefficients (Ohja & Hibbert 1987;Keenan et al 1993) which are included in the present study. In our photoionisation cross-section calculations for this element, all 512 levels arising from the eight configurations: 3s 2 3p 3 , 3s3p 4 , 3s 2 3p 2 3d, 3s 2 3p3d 2 , 3s3p 3 3d, 3p 3 3d 2 , 3p 5 , 3s3p 2 3d 2 of the residual chlorine doubly ionized ion were included in the close-coupling expansion.…”
Absolute photoionisation cross sections for the Cl + ion in its ground and the metastable states; 3s 2 3p 4 3 P 2,1,0 , and 3s 2 3p 4 1 D 2 , 1 S 0 , were measured recently at the Advanced Light Source (ALS) at Lawrence Berkeley National Laboratory using the merged beams photon-ion technique at an photon energy resolution of 15 meV in the energy range 19 -28 eV. These measurements are compared with large-scale Dirac Coulomb R-matrix calculations in the same energy range. Photoionisation of this sulphur-like chlorine ion is characterized by multiple Rydberg series of autoionizing resonances superimposed on a direct photoionisation continuum. A wealth of resonance features observed in the experimental spectra are spectroscopically assigned and their resonance parameters tabulated and compared with the recent measurements. Metastable fractions in the parent ion beam are determined from the present study. Theoretical resonance energies and quantum defects of the prominent Rydberg series 3s 2 3p 3 nd, identified in the spectra as 3p → nd transitions are compared with the available measurements made on this element. Weaker Rydberg series 3s 2 3p 3 ns, identified as 3p → ns transitions and window resonances 3s3p 4 ( 4 P )np features, due to 3s → np transitions are also found in the spectra.
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